scholarly journals Heavy-to-Light Form Factors in the Quark Model with Infrared Heavy-Quark Propagators

1998 ◽  
Vol 24 (4) ◽  
pp. 201-212 ◽  
Author(s):  
M. A. Ivanov ◽  
T. Mizutani ◽  
Yu. M. Valit

1997 ◽  
Vol 56 (11) ◽  
pp. 7089-7104 ◽  
Author(s):  
Dmitri Melikhov


1994 ◽  
Vol 412 (1-2) ◽  
pp. 169-180 ◽  
Author(s):  
F.E. Close ◽  
A. Wambach


1999 ◽  
Vol 451 (1-2) ◽  
pp. 187-194 ◽  
Author(s):  
J. Charles ◽  
A. Le Yaouanc ◽  
L. Oliver ◽  
O. Pène ◽  
J.-C. Raynal


1997 ◽  
Vol 12 (09) ◽  
pp. 653-660 ◽  
Author(s):  
M. A. Ivanov ◽  
Yu. M. Valit

The q2-dependence of the heavy-to-light form factors in the full physical region is obtained within the relativistic quark model with heavy infrapropagators. It is shown that the behavior of the vector form factors agrees with the pole dominance hypothesis whereas the behavior of the axial form factors is rather different from the polelike function.





1969 ◽  
Vol 11 (1) ◽  
pp. 61-68 ◽  
Author(s):  
M. Böhm ◽  
D. Rein


2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Junegone Chay ◽  
Chul Kim

Abstract In soft-collinear effective theory, we analyze the structure of rapidity divergence due to the collinear and soft modes residing in disparate phase spaces. The idea of an effective theory is applied to a system of collinear modes with large rapidity and soft modes with small rapidity. The large-rapidity (collinear) modes are integrated out to obtain the effective theory for the small-rapidity (soft) modes. The full SCET with the collinear and soft modes should be matched onto the soft theory at the rapidity boundary, and the matching procedure becomes exactly the zero-bin subtraction. The large-rapidity region is out of reach for the soft mode, which results in the rapidity divergence. The rapidity divergence in the collinear sector comes from the zero-bin subtraction, which ensures the cancellation of the rapidity divergences from the soft and collinear sectors. In order to treat the rapidity divergence, we construct the rapidity regulators consistently for all the modes. They are generalized by assigning independent rapidity scales for different collinear directions. The soft regulator incorporates the correct directional dependence when the innate collinear directions are not back-to-back, which is discussed in the N-jet operator. As an application, we consider the Sudakov form factor for the back-to-back collinear current and the soft-collinear current, where the soft rapidity regulator for a soft quark is developed. We extend the analysis to the boosted heavy quark sector and exploit the delicacy with the presence of the heavy quark mass. We present the resummed results of large logarithms in the form factors for various currents with the light and the heavy quarks, employing the renormalization group evolution on the renormalization and the rapidity scales.



2001 ◽  
Vol 511 (1) ◽  
pp. 33-39 ◽  
Author(s):  
R.F. Wagenbrunn ◽  
S. Boffi ◽  
W. Klink ◽  
W. Plessas ◽  
M. Radici


2004 ◽  
Vol 2004 (07) ◽  
pp. 081-081 ◽  
Author(s):  
Richard J Hill ◽  
Thomas Becher ◽  
Seung J Lee ◽  
Matthias Neubert
Keyword(s):  


Sign in / Sign up

Export Citation Format

Share Document